Method and system for microfluidic particle orientation and/or sorting

ABSTRACT

A system for orienting particles in a microfluidic system includes one or more radiation pressure sources arranged to expose particles to radiation pressure to cause the particles to adopt a particular orientation in the fluid. A system for sorting particles in a microfluidic system includes a detection stage arranged to detect at least one difference or discriminate between particles in the fluid flow past the detection stage, and one or more radiation pressure sources past which the particles move sequentially and a controller arranged to switch radiation energy to cause a change in direction of movement of selected particles in the fluid flow to sort the particles. The particles may be biological particles such as spermatazoa. The radiation pressure may be optical pressure and may be from one or more waveguides which may extend across a channel of the microfluidic system.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a Continuation of U.S. Ser. No. 16/507,752, filedJul. 10, 2019 which is a continuation of U.S. Ser. No. 15/697,770, filedSep. 7, 2017 which is a divisional application of U.S. Ser. No.14/417,622, filed Jan. 27, 2015, which is a national stage application,filed under 35 U.S.C. 371, of International Application No.PCT/NZ2013/000135, filed Jul. 29, 2013, which claims the benefit of, andpriority to, U.S. Ser. No. 61/676,391, filed Jul. 27, 2012. The contentsof each of these applications is incorporated by reference in theirentirety.

FIELD OF INVENTION

The invention relates to a method and system for particle orientationand/or sorting in a micro fluidic system.

BACKGROUND

Developments in commercial and academic medical and biotechnology havedriven a strong focus on methods for biological cell sorting. The twomain approaches that have emerged—bulk separation and single cellsorting—both enrich a population of cells with a targeted subset withspecific physicochemical (i.e. size, volume, light scatteringproperties, etc.), immunological, or functional characteristics. Bulksorting generally focuses upon a single discriminating cellular feature.Examples include cell filtration, centrifugation/sedimentation andaffinity-based panning methods. The main disadvantages of bulk sortingare lower purity, loss of cells during the sorting process, difficultyin sorting out relatively rare cells, and difficulty in discriminatingamong similar sub-populations of cells. Bulk sorting, however, is arelatively simple method that offers high throughput. In contrast,single cell methods, the most important of which is fluorescenceactivated cell sorting (FACS) by flow cytometry, examine each cellindividually to target the desired subpopulation for isolation and thenguide them into different output streams. The reduction in throughput isoffset by major advantages in specificity of sorting that is tunable tothe desired outcome, generally higher recovery of cells, the ability tosort rare or only weakly discriminated cell populations, and theavailability of multi-target sorting based on an array of multiplecellular features (i.e. several types of surface receptor, each taggedwith a different fluorescent label). One important challenge faced byFACS flow cytometric methods is the damage incurred by some cells in theflow (shear stress) and sorting (electric field damage) processes. Animportant example is the reduced fertility of sorted sperm samples thatcan be attributed to these disruptive physical processes.

In the agriculture sector, cell discrimination is particularly importantin livestock species where artificial insemination is commonly practisedsuch as cattle. The use of sexed semen facilitates control o f offspringgender for commercial benefit. The current commercially important methodfor sperm sorting uses FACS flow cytometry, in which sperm arediscriminated by their differences in DNA content. The DNA of eachspermatazoon is stained with a fluorescent dye in proportion to the DNAcontent. As the X chromosome is larger (i.e. has more DNA) than the Ychromosome, the “female” (X-chromosome bearing) spermatozoa will absorba greater amount of dye than the “male” (Y-chromosome bearing)spermatozoa and as a consequence when exposed to UV light during flowcytometry will fluoresce with higher intensity than the Y spermatozoa.Before detection or discrimination the sperm may be orientedhydrodynamically and the sperm may be separated into individual dropletsthat then may be electrically charged. After detection ordiscrimination, the sperm are sorted by electric field—charged dropletinteractions.

SUMMARY OF THE INVENTION

In broad terms in one aspect the invention comprises a method oforienting particles in a microfluidic system, which includes exposingthe particles to radiation pressure in a microfluidic system to cause atleast a majority of the particles to adopt a particular orientation inthe fluid.

In broad terms in another aspect the invention comprises a system fororienting particles in a microfluidic system, which includes one or moreradiation pressure sources arranged to expose particles in themicrofluidic system to radiation pressure to cause at least a majorityof the particles to adopt a particular orientation in the fluid.

The particles may be biological or non-biological particles. Typicallythe particles are asymmetric particles. The asymmetry may be in anyphysical property that leads to an asymmetric interaction with theincident radiation, including but not limited to asymmetry in physicaldimensions of the particles. In some embodiments the particles may besperm, red blood cells, or bacteria, for example.

The radiation pressure may be optical pressure and may be from one ormore waveguides which may extend across a channel of the microfluidicsystem, for example across above, below or across the side walls of thechannel, or may abut a channel from above, below or the side. Thewaveguide(s) may be one or more optical waveguides are connected to alight source, such as a laser, to transport light and generate theradiation pressure also referred to as optical force, photon pressure orelectromagnetic pressure. The one or more waveguides may be manufacturedas part of the intrinsic process of fabricating the microfluidic system,or may be inserted as fibre optic units in the construction of the finalsystem.

A microfluidic system for orienting particles as above may also comprisea pre-stage for focusing and/or singulating the particles into aparticular location within the channel. This system may be hydrodynamicor radiation pressure based.

In broad terms in another aspect the invention comprises a method ofsorting particles in a microfluidic system, which includes:

-   -   detecting at least one difference or discriminating between        particles, and    -   switching based on an input from the detection or        discrimination, one or more radiation pressure sources past        which the particles move sequentially to cause a change in        direction of movement of selected particles in the fluid flow to        sort the particles.

The particles may be directed into two or more than two differentoutputs.

The one or more radiation pressure sources may be one or morewaveguides, which may extend across a channel of the microfluidicsystem, for example across above, below or across the sidewalls of thechannel, or may abut a channel from above, below or the side.

The step of detecting at least one difference or discriminating betweenparticles may comprise an optical technique for assessing acharacteristic of the particle, the technique may be afluorescence-based detection technique.

The method may also comprise singulating particle flow and may alsocomprise focusing the particles to a particular location within thechannels. The forces may be hydrodynamic or radiation pressure based.

The method may also comprise causing at least a majority of theparticles to first adopt a particular orientation in the fluid beforedetecting, where the particles are asymmetric particles.

The orientation step may comprise exposing the particles to radiationpressure such as optical pressure to cause at least a majority of theparticles to adopt a particular orientation in the fluid.

In broad terms in another aspect the invention comprises a system forsorting particles in a microfluidic system, which includes:

-   -   a detection stage arranged to detect at least one difference or        discriminate between particles in the fluid flow past the        detection stage, and    -   one or more radiation pressure sources past which the particles        move sequentially and a controller arranged to switch based on        an input from the detection or discrimination stage, radiation        energy in the one or more radiation pressure sources to cause a        change in direction of movement of selected particles in the        fluid flow to sort the particles.

The system may be arranged to switch or sort the particles so that eachparticle is directed into one of two or one of more than two differentoutputs.

The one or more radiation pressure sources may be one or more waveguideswhich may extend at least partway across a channel of the microfluidicsystem, for example across above, below or across the side walls of thechannel, or may abut the channel from above, below or the side.

The detection stage may be arranged to detect or discriminate particlesby an optical technique such as a fluorescence-based detectiontechnique.

The particles may be biological or non-biological particles. Typicallythe particles are asymmetric particles. The asymmetry may be in anyphysical property that leads to an asymmetric interaction with theoptical force, including but not limited to asymmetry in physicaldimensions. In some embodiments the particles may be sperm, red bloodcells, bacteria, or nanoparticles for example.

A microfluidic system for orienting particles as above may also comprisea pre-stage singulating particle flow and may also comprise a pre-stagefor focusing the particles into a particular location within thechannel. This system may be hydrodynamic or optical.

The system may also comprise an orientation stage arranged to cause atleast a majority of the particles to first adopt a particularorientation in the fluid, particularly where the particles areasymmetric particles. The orientation stage may comprise one or morewaveguides arranged to in use expose particles to radiation such asoptical pressure to cause at least a majority of the particles to adopta particular orientation in the fluid.

In broad terms in another aspect the invention comprises a microfluidicsystem for sexing sperm which includes:

-   -   one or more orienting radiation pressure sources arranged to        expose sperm to pressure to cause individual sperm to adopt a        common orientation in the fluid    -   a fluorescence-based detection stage arranged to discriminate        male and female sperm in the fluid flow past the detection        stage, and    -   one or more switching radiation pressure sources s past which        the individual sperm subsequently move, and    -   a controller arranged receive an input from the detection stage        and to control radiation energy in the one or more switching        radiation pressure sources to separately direct male and/or        female sperm.

A microfluidic system for orienting particles as above may also comprisea pre-stage for singulating sperm flow and a pre-stage for focusing thesperm into a particular location within the channel. This system may behydrodynamic or optical.

The term “comprising” as used in this specification means “consisting atleast in part of”. When interpreting statements in this specificationwhich include that term, the features prefaced by that term in eachstatement all need to be present but other features can also be present.Related terms such as “comprise” and “comprised” are to be interpretedin the same manner.

BRIEF DESCRIPTION OF THE DRAWINGS

The invention is further described with reference to the accompanyingfigures in which:

FIG. 1 schematically illustrates an embodiment of a microfluidic systemof the invention for particle sorting,

FIGS. 2a and 2b schematically illustrate embodiments for particleorientation in which a single waveguide—FIG. 2a , or multiplewaveguides—FIG. 2b , abut the microchannel from above, below or from aside of the channel,

FIGS. 3a and 3b schematically illustrate embodiments for particleorientation in which a single waveguide—FIG. 3a , and multiplewaveguides—FIG. 3b , extend across the microchannel above, below oralong a side wall of the channel,

FIGS. 4a and 4b schematically illustrate embodiments for sorting orswitching selected particles in a fluid flow in a microchannel, in whichmultiple waveguides abut the channel from above, below or from a side ofthe channel,

FIGS. 5a and 5b schematically illustrate embodiments for sorting orswitching selected particles in a fluid flow in a microchannel, in whichmultiple waveguides extend across the channel above, below or along theside wall of the channel,

FIG. 6a shows an embodiment of a microfluidic chip the invention forperforming orientation and separation of sperm and FIG. 6b shows anarray of individual sorting chips may arranged for massively parallelmicrofluidic implementation to sort sperm according to sex,

FIGS. 7a and 7b are computational geometries used in FEM simulationsreferred to on the subsequent description of experimental work, FIG. 7a—elliptical cylinder in water placed along the optical axis of waveguide40 μm from terminus of waveguide and FIG. 7b —elliptical cylinder placedabove an SU8 photo-epoxy waveguide with a small gap separating thecylinder from the waveguide,

FIG. 8 shows torque on elliptical cylinder in water at a variety ofdistances from the terminus of a waveguide, referred to on thesubsequent description of experimental work,

FIG. 9 shows torque on an elliptical cylinder in water above a waveguideat 3 separation distances, referred to on the subsequent description ofexperimental work,

FIG. 10 shows Fx and Fy forces on an elliptical cylinder in water at theterminus of a waveguide in the vertical orientation for a variety ofseparation distances, referred to on the subsequent description ofexperimental work,

FIG. 11 shows Fx and Fy optical forces on an elliptical cylinder inwater above a waveguide for a variety of separation distances, referredto on the subsequent description of experimental work,

FIGS. 12a-c show symmetrical particle displacement by an optical fieldas the particle flows past the end of a wave-guide terminus in amicrofluidic channel referred to on the subsequent description ofexperimental work,

FIGS. 13a and b show an asymmetrical particle displacement by, andoriented by an optical field as the particle flows past the end of awave-guide terminus in a microfluidic channel, referred to on thesubsequent description of experimental work, and

FIG. 14 shows the measured displacement efficiency as a function ofparticle flow speed for symmetric particles—FIG. 14a , and asymmetricparticles—FIG. 14 b.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Referring to FIG. 1 the microfluidic system typically provided on amicrofluidic chip for particle orientation and sorting comprisesfocusing, orientation, detection of a discriminating feature that may befluorescence, and timing and switching stages sequentially along amicrochannel along which the particles move with the fluid flow in thechannel, from one stage to the next.

In the embodiment shown a hydrodynamic focusing and/or singulating stage1 places the particles in a particular location in the channel.

If the particles are asymmetric, such as sperm for example, the initialorientation of the particles may be random, and an orientation stage 2orients the particles substantially all or at least a majority with acommon orientation predetermined relative to the channel geometry. Inthe schematic figure the particles are shown being oriented vertically.In a preferred embodiment the particles are oriented at the orientationstage by optical forces such as from an optical waveguide as will befurther described. One or more waveguides may extend across the channel,for example across above, below or along the side wall of the channel,or may abut the channel from above, below or from the side of thechannel. The waveguide may form part of the channel wall, or may bephysically separated from the microfluidic chamber.

In this embodiment the detection stage 3 is a fluorescence-baseddetection stage and the particles are previously stained with afluorescent dye, and the fluorescence detection stage 3 evaluates thefluorescence intensity of each particle and passes fluorescenceinformation to timing and switching stages 4 and 5, which switch or sortthe particles so that each particle is directed into one of twodifferent outputs 6 and 7. The timing and switching stages 4 and 5 arecontrolled by an electronic controller 15. For example the particles maybe sperm and male sperm may be directed to output 6 and female sperm tooutput 7 for example. Alternatively particles may be sorted to selectone particle type which is desired from another particle type which isnon-desired for the particular application, such as to select red bloodcells for example and in such an embodiment the desired particles may bedirected to collection or to further processing while the undesiredparticles may be directed to waste or an outlet to waste or some otherprocessing.

The particles enter the microfluidic system from source 8. In the figurethe source 8 and outputs 6 and 7 are schematically shown as collectionvolumes such as chambers for containing the particles, but the particlesmay enter the system or the sorting section of the microfluidic system,from a microfluidic channel or channels from a prior processing stageand exit the sorting section to microfluidic channels carrying theparticles to other subsequent processing for example.

FIGS. 2a and 2b schematically illustrate embodiments for particleorientation in which a single waveguide—FIG. 2a , or multiplewaveguides—FIG. 2a , abut the microchannel from a side (above, below orfrom either side) of the channel, which may be used in the orientationstage 2 of the system of FIG. 1. In FIG. 2a , a radiation waveguide 9such as an optical fibre connected to a source such as a laser abuts thechannel from one side of the channel. The waveguide may form part of thewall of the channel or may be physically separated from the microfluidicchamber. As asymmetric particles in random orientation pass the terminusof the waveguide 9, they are subjected to an optical force which tendsto cause the asymmetric particles to orient with a common andpredetermined orientation. In the embodiment of FIG. 2b , the particlespass three waveguides 9 a-9 c in a series, which cumulatively orient theparticles. The optical force from the first waveguide 9 a may cause eachparticle to begin rotating towards a desired orientation, while opticalforce from subsequent waveguides 9 b and 9 c continues to cause theparticle to move to the desired orientation. FIG. 2a shows a singlewaveguide abutting the side of the channel and FIG. 2b three waveguidesabutting the side of the channel but alternative embodiments maycomprise two or more than three waveguides, and the waveguides may abutthe channel from above, below or from either side.

Waveguides may be manufactured as part of the device (i.e. in situ) orinserted during device assembly (i.e. fibre optic components). Typicallythe waveguides may apply optical force in an optical wavelength rangefrom the visible to near-infrared (500 nm-2 μm), and laser light sourceswill be CW emission sources with output powers of less than 1W/waveguide, to minimise the optical forces applied in each interactionwith the particle. The emission of the laser light may be controlledelectronically, to switch on and off as desired to generate pulses onthe microsecond to millisecond timescale.

FIGS. 3a and 3b schematically illustrate embodiments for particleorientation in which a single waveguide 10 a-FIG. 3a , and multiplewaveguides 10 a-10 d—FIG. 3b , extend across the microchannel above orbelow the channel. The waveguide(s) extend above, below or along a sidewall of the microchannel so that the particles pass by the waveguides,and in doing so are subject to radiation emanating from the waveguidesand which applies photon pressure to orient the particles describedabove. Optical radiation may be supplied to the waveguide(s) from acoupling lens 12 as shown.

An advantage of the waveguide-based orientation embodiments describedabove, over particle orientation via hydrodynamic pressure as commonlyused in sperm sexing with conventional flow cytometry for example, isthat less force is applied to the particles such as sperm to orientthem, so that there is a lower likelihood of particle damage during oras a result of the particle orientation. This may be particularly so forthe embodiments of FIGS. 2b and 3b which orient the particles via aseries of sequential waveguides each applying lower radiation pressurethan would be required to orient the same particles with radiationpressure from a single waveguide. This may be particularly advantageousfor biological particles such as sperm, and cells for example.

FIGS. 4a and 4b show an embodiment for sorting or switching selectedparticles to change the direction of movement in the fluid flow in themicrochannel, in which the multiple waveguides 11 a-11 e abut thechannel from a side of (or above or below) the channel. FIGS. 5a and 5bshow an embodiment for sorting or switching selected particles to changethe direction of movement in the fluid flow in the microchannel, inwhich the multiple waveguides extend across the channel above, below oralong side of the channel. After the fluorescence detection stage 3(FIG. 1), in the switching stage 4 (FIG. 1) each particle passes aseries of waveguides 11 a-11 e which enter the microchannel from theside in FIG. 4a and 4b , or 13 a-13 d which pass below or above themicrochannel in the embodiment of FIGS. 5a and 5b . The waveguides inFIGS. 4a, 4b, 5a and 5b may form part of the wall of the channel or maybe physically separated from the microfluidic chamber.

Referring to FIGS. 4a and 5a , when a particle desired to be switched toa particular output 6 or 7 passes through the switching stage 5 (seeFIG. 1), the energy source to each of the waveguides Ha-He or 13 a-13 dis switched on. As the particle passes the first waveguide, it isdeflected by the optical force, and is further deflected as it passesthe subsequent waveguides. All of the waveguides may be energisedtogether, from a common laser source through a coupling lens 12 as shownin FIGS. 5a and 5b for example, or in a higher speed system particlemovement may be timed with switching of each of waveguides 11 a-11 e or13 a-13 d so that each waveguide is energised, one after the other, asthe selected particle passes each individual waveguide. Controller 6(see FIG. 1) with input(s) from timing stage 4 (see FIG. 1) sequencesthe energising of the switching waveguides with the passing theswitching stage of the selected particles. In the embodiment shown,there is a laminar flow through the channel and, referring to FIGS. 4aand 5a , the waveguides when energised act to deflect selected particlesfrom the flow on one side towards output 7 across the flow boundary andinto the flow towards output 6. When the waveguides are not excited,there is no deflection of the particles which therefore continue movetowards output 7, as shown in FIGS. 4b and 5b . In the embodiments shownthe system is arranged to switch or sort the particles so that eachparticle is directed into one of two outputs 6 and 7 but in alternativeembodiments the system may be arranged to switch or sort the particlesbetween more than two different outputs such as three or four outputsfor example. For example the waveguides when sequentially energised maydeflect selected particles from the flow on one side across a first flowboundary and into a second flow and then across a second flow boundaryand into a third flow towards a third output. Switching or sorting maybe based on ternary rather than binary characteristics of the particlesfor example. Also in alternative embodiments the waveguides may operateto cause selected particles to deflect to turn into a different channelor channels instead of collection volumes for example.

FIG. 6a shows a microfluidic chip that incorporates an embodiment of theinvention to perform orientation and separation of bovine sperm. Thesperm sample, with DNA already stained and rinsed, enters the chip atSample in, along with two sheath fluid flows Sh. The sperm sample andsheath flows are cooled by a Peltier cooling stage (not shown) beneaththe chip, and maintained at low temperature throughout the on-chipprocessing. The sperm are focused into the desired region of the channelin region FF. They are then oriented at O using the radiation pressurefrom a fibre bank FB1. In this example, the fibre bank abuts the channelfrom the side and four single-mode fibres are shown. These fibrestransmit light from a laser into the chip. After orientation, thefluorescence intensity of the sperm DNA is evaluated using a UV LED L1illuminating the detection region from beneath the chip. Thefluorescence is coupled out of the channel using single mode fibre SMFand sent to photomultiplier tube detector PMT. The output ofphotomultiplier tube detector PMT is used to control switching systemSw. If a sperm is selected to be directed to a new output channel, thelaser sends light through second fibre bank FB2 to move the sperm in thechannel to a new flow stream. The sperm then flow across a secondthermal gradient to raise the temperature in a controlled fashion to adesired temperature Such as room or body temperature—note that theserpentine path required for thermal equilibrium with the gradient isnot shown for the output channels for clarity. The output channels alsoinclude flow outputs for the sheath fluid and a waste stream, as well asfor the X- and Y-chromosomal sperm. A white light source L2 beneath theoutput channels induces scattering from particles that enter theindividual output channels. That scattering is detected using a thirdbank of fibres FB3 so that the sperm switching can be detected by Si PINdiodes and sent to the controller for counting.

FIG. 6b shows how an array of individual sorting chips may be used toachieve bulk sorting of sperm samples. The controlling electronics,laser sources, sensors, driver for the Peltier stage (T-control) andbulk fluid input and output flow are external to the sorting chip. Inthis diagram, only four chips are shown, for clarity only.

Again an advantage of the waveguide-based particle switching embodimentsdescribed above, over particle switching via hydrodynamic pressure forexample, is that less force is applied to the particles, and this may beparticularly advantageous for biological particles such as sperm andcells for example. Thus while a waveguide-based particle switching stageas described above may be preceded by a hydrodynamic pressure-basedparticle orientation stage (if a particle orientation stage isrequired), and vice versa a waveguide-based particle orientation stageas described above may be followed by a hydrodynamic particle switchingstage, in a preferred embodiment a system particularly for sortingasymmetric biological particles such as sperm may comprise awaveguide-based orientation stage arranged to orient the sperm byradiation pressure, a detection stage such as a fluorescence-baseddetection stage, and a waveguide-based switching stage which usesoptical force to separately direct male and female sperm. The systemwill also have an electronic such as a microprocessor-based controlsystem. The fluorescence detection stage 3 may be arranged to irradiatethe sperm previously contacted or stained with a fluorescent marker dyewhich binds to the DNA of each spermatozoom, and comprises a detector todetect the intensity of the resulting fluorescence. The female absorb agreater amount of dye than the male sperm, and therefore fluoresce withhigher intensity and enabling discrimination.

Systems which are comprised of only a single waveguide are restricted intheir processing speed by the limited impulse (force×time) of theoptical force on the particle of interest. The interaction time islimited by the physical size of the waveguide and the flow speed of theparticles. The manipulation force is limited by the optical trappingpotential of the waveguide. Higher forces lead to complete opticaltrapping, in which particles are no longer free to move with thesurrounding fluid. This sets the typical use of single waveguideparticle manipulation to low throughput, high precision processing ofparticles. Multiple waveguide orientation and switching embodiments,such as described above offer the advantage of continuous application ofa well controlled optical force over an extended time without theoccurrence of optical trapping. This allows for arbitrarily highthroughput (particle flow speed) of particles by the serial addition ofoptical force producing waveguides increasing the impulse applied to theparticle.

A microfluidic system of the invention for sorting sperm or theparticles may have at least one microchannel with a sorting section inwhich the particles are processed as described above, or arrays of suchsorting sections to increase throughput. Systems are preferably embodiedin a small microfluidic device or chip prepared by micromachining,polymer processing techniques or other microfabrication technologies toform the microfluidic structures, and comprises supporting pumps,valving and instrumentation. Typically the microchannel(s) may have awidth in the range 10 to 500 microns, or 100 to 400 microns, and a depthin the range 5 to 250 microns, for example. The dimensions of themicrofluidic flow channels support laminar flow, with minimalturbulence. In the embodiments described and illustrated in the figures,the microstructure has a planar form with in-plane length and widthgreater than depth transverse to the plane. In alternative embodiments,the depth may be greater than the length and/or width of themicrochannel and reservoir and other cavities of the microsystem. Inalternative embodiments, the microchannels may extend in threedirections, and may feature curved segments as well as angles. In theembodiments shown in the figures the microcavities have a rectangular orsquare cross-section but in alternative embodiments the microstructuresmay have a circular or oval cross-section for example, or across-section of other shape.

EXPERIMENTAL

The invention is further illustrated by way of example by the followingdescription of simulation and trials work.

Example 1

Simulations were conducted using the finite element method (FEM) toapproximate the action of optical forces on asymmetric particles.Specifically, the optical forces applied to elliptical particlessituated near waveguides such as those described above were calculated.The orienting angular torques were calculated and thetrapping/propulsive forces were also calculated. 2-dimensional (2D)approximations of elliptical particles (a cylinder) with a 10 μm:2 μmmajor:minor axis were placed at the terminus of the 2D approximation ofa single mode optical optical fiber, a slab waveguide—FIG. 7a . Theresulting torque applied to such an elliptical particle as a function ofits orientation with respect to the waveguide optical axis is shown inFIG. 7b . The applied input power in the waveguide is 50 mW. Waveguidemodes polarized parallel (TM) and perpendicular to (TE) the plane ofsimulation are shown. The same 2D particle approximation was placedabove a 2D approximation of a ridge waveguide, as shown in FIG. 8, andthe resulting torque as a function of orientation parallel to thewaveguide optical axis is shown in FIG. 9. Both results show that theparticle is oriented (has no applied torque) when its minor axis isparallel to the optical axis of the waveguides. That is, when it is inthe vertical (angle=90°) orientation. Further the graphs show that thetorque is restoring (in opposition to direction of motion) about thatorientation angle. This is equilibrium orientation of the particle dueto the applied optical forces. The resulting optical force applied tothe above elliptical cylinder in water when at the terminus of awaveguide is shown in FIG. 10. The optical force applied to the sameelliptical cylinder in water when above a waveguide is shown in FIG. 11.These optical forces are shown separated into direction parallel to (Fx)and perpendicular to (Fy) the waveguide optical axes for a variety ofparticle/waveguide separations for both TM and TE polarized waveguidemodes. The particles are in the vertical/equilibrium orientation asdescribed above.

Example 2

The images of FIGS. 12a-c which show symmetrical particle displacementby an optical field as a particle P moved past the end of a wave-guideterminus W in a 100 μm wide rectangular microfluidic channel flow F werecollected with a 10× microscope objective imaged onto a CMOS digitalcamera sensor. The particle was a 10 μm diameter polystyrene sphericalbead, and is shown flowing from top to bottom in FIG. 12. FIG. 12a showsthe particle in the fluid flow before the waveguide. The particleinteracted with the optical beam (250 mW of 532 nm coupled into a singlemode fibre at >50% efficiency) diverging from the waveguide terminus.This interaction generated the strong scattering seen saturating theimage of FIG. 12b . The optical force pushed the particle bydisplacement d as shown in FIG. 12c without stopping the flow of theparticle along the microfluidic channel.

Example 3

FIG. 13 illustrates the orienting effects of the optical field at theterminus of a waveguide W adjacent to the wall of a microfluidicchannel. A particle P with an asymmetric shape specifically a bovinespermatozoa, was carried in a fluid flow from top to bottom in a fluidflow F in a microfluidic channel. The particle was inert and unable tomove under its own propulsion. As shown in FIG. 13a the spermatozoainitially presented a dark scattering orientation to the imaging system.After passing through and interacting with the optical field at theterminus of the optical waveguide (outlined in FIG. 13) the spermatozoacontinued to flow down the microfluidic channel with a new orientationand a displacement from its initial position. The particle was movedaway from the channel wall after the interaction and rotated to a neworientation, but continued to flow down the channel. The new orientationof the spermatozoa presented a white head, indicating a rotation of 90degrees about the long axis of the particle after interacting with theoptical field.

Multiple interaction events such as those observed in FIG. 12 and FIG.13 were analysed frame-by-frame and the results presented in FIG. 14.Image processing was used to measure the particle position andorientation before and after interacting with the optical field. FIG. 14shows the measured displacement efficiency as a function of particleflow speed for symmetric particles namely a 10 μm diameter polystyrenebead—FIG. 14a , and asymmetric particles namely non-motile bovinespermatozoa—FIG. 14b . For example these particles are flowing past theterminus of a single waveguide with less than 200 mW output power at awavelength of 532 nm. Offset indicates distance from fibre terminationto the edge of the microfluidic channel.

1-30. (canceled)
 31. A particle orientation system for orientingparticles in a microfluidic system, comprising one or more radiationpressure sources arranged to expose asymmetric particles in themicrofluidic system to radiation pressure to cause at least a majorityof the particles to adopt a particular orientation in the fluid.
 32. Thesystem of claim 31, further comprising one or more waveguides arrangedto expose particles to the radiation pressure from the one or moreradiation pressure sources.
 33. The system of claim 31, wherein the oneor more radiation pressure sources are configured as a particleorientation stage.
 34. The system of claim 33, further comprising amicrofluidic channel configured to receive and flow the plurality ofparticles, wherein the orientation stage arranged at least one of on oradjacent the microfluidic channel.
 35. The system of claim 33, furthercomprising a singulating stage arranged to singulate particles in thefluid prior to the orientation stage.
 36. The system of claim 34,further comprising a singulating stage arranged to singulate particlesin the fluid prior to the orientation stage.
 37. The system of claim 34,further comprising a focusing stage configured to focus the plurality ofparticles to a particular location within the microfluidic channel. 38.The system of claim 31, wherein the particles are biological particles.39. The system of claim 38, wherein the particles are sperm.
 40. Thesystem of claim 31, wherein the particles are sperm.
 41. A method fororienting particles in a microfluidic system comprising exposing aplurality of particles flowing in a microfluidic channel to radiationpressure from one or more radiation pressure sources to cause at least amajority of the particles to adopt a particular orientation in thefluid.
 42. The method of claim 41, wherein the microfluidic channel isexposed to radiation pressure from the one or more radiation pressuresources via one or more waveguides.
 43. The method of claim 41, furthercomprising singulating the plurality of particles flowing in themicrofluidic channel.
 44. The method of claim 41, wherein the particlesare biological particles.
 45. The method of claim 44, wherein thebiological particles are sperm.
 46. The method of claim 41, wherein theparticles are sperm.